Reuse & Permissions

It is not necessary to obtain permission to reuse this article or its components as it is available under the terms of the Creative Commons Attribution 4.0 International license. This license permits unrestricted use, distribution, and reproduction in any medium, provided attribution to the author(s) and the published article's title, journal citation, and DOI are maintained. Please note that some figures may have been included with permission from other third parties. It is your responsibility to obtain the proper permission from the rights holder directly for these figures.

Export citation

Export citation

Choose format for download:

Download Citation
  • Open Access

Self-gravitating quantum stars with a globally relevant Bohm potential

Ilídio Lopes

Phys. Rev. D 113, 115043 – Published 16 June, 2026

DOI: https://doi.org/10.1103/m6jf-8cyl

Abstract

The microphysics underlying nonbaryonic dark matter remains unknown. I derive the two-species Schrödinger-Poisson-Yukawa system for spin-12 dark-sector fermion fields, ψ (mass m1) and χ (mass m2), coupled through a scalar mediator of mass mϕ via a universal Yukawa coupling, within an orbital-free density-functional framework with the Kirzhnits gradient coefficient λB=1/9. A central result is that the Bohm potential, far from being negligible in the Thomas-Fermi regime, contributes a species-dependent surface-energy correction analogous to the nuclear liquid-drop model; the heavier fermion species generates an outward quantum-pressure wall whilst the lighter species provides an inward surface tension, with degeneracy pressure furnishing the bulk confinement. In the single-species Schrödinger-Poisson limit the ground state recovers the benchmarked invariants Mdim≃3.883 and xT≃2.562, yielding MRT≃9.95λBℏ2/(Gm12). For polytropic index γ=5/3 the mass-radius relation satisfies R∝M−1/3; for γ=4/3 a limiting mass emerges above which no stable equilibrium exists. Illustrative configurations span M=10−8–5M⊙, m1∼10−14−10−6  eV, and radii from a few km to ∼103R⊙, with gravitational-wave contact frequencies in the Einstein Telescope and LISA bands and microlensing signatures accessible to current surveys. The predictive rigidity of the resulting mass-radius relation, in which the single microphysical parameter m1 determines the equilibrium radius once the total mass is specified, furnishes a reproducible, first-principles reference for constraining the dark-fermion mass in multicomponent dark sectors.

View figure in article

Physics Subject Headings (PhySH)

Article Text

References (91)

  1. N. Aghanim, Y. Akrami, M. Ashdown, J. Aumont, C. Baccigalupi, M. Ballardini, A. J. Banday, R. B. Barreiro, N. Bartolo et al. (Planck Collaboration), Planck 2018 results. VI. Cosmological parameters, Astron. Astrophys. 641, A6 (2020).
  2. J. S. Bullock and M. Boylan-Kolchin, Small-scale challenges to the ΛCDM paradigm, Annu. Rev. Astron. Astrophys. 55, 343 (2017).
  3. J. F. Navarro, C. S. Frenk, and S. D. M. White, The structure of dark matter halos, Astrophys. J. 462, 563 (1996).
  4. S. Navas et al. (Particle Data Group), Review of particle physics, Phys. Rev. D 110, 030001 (2024).
  5. D. N. Spergel and P. J. Steinhardt, Observational evidence for self-interacting cold dark matter, Phys. Rev. Lett. 84, 3760 (2000).
  6. W. Hu, R. Barkana, and A. Gruzinov, Fuzzy cold dark matter: The wave properties of ultralight particles, Phys. Rev. Lett. 85, 1158 (2000).
  7. D. J. E. Marsh, Axion cosmology, Phys. Rep. 643, 1 (2016).
  8. E. G. M. Ferreira, Ultra-light dark matter, Astron. Astrophys. Rev. 29, 7 (2021).
  9. L. Hui, J. P. Ostriker, S. Tremaine, and E. Witten, Ultralight scalars as cosmological dark matter, Phys. Rev. D 95, 043541 (2017).
  10. H.-Y. Schive, T. Chiueh, and T. Broadhurst, Cosmic structure as the quantum interference of a coherent dark wave, Nat. Phys. 10, 496 (2014).
  11. H.-Y. Schive, T. Chiueh, T. Broadhurst, and K.-W. Huang, Contrasting galaxy formation from quantum wave dark matter, ψDM, with ΛCDM, Phys. Rev. Lett. 113, 261302 (2014).
  12. D. J. Kaup, Klein-Gordon geon, Phys. Rev. 172, 1331 (1968).
  13. R. Ruffini and S. Bonazzola, Systems of self-gravitating particles in general relativity and the concept of an equation of state, Phys. Rev. 187, 1767 (1969).
  14. S. L. Liebling and C. Palenzuela, Dynamical boson stars, Living Rev. Relativity 26, 1 (2023).
  15. E. H. Lieb, Existence and uniqueness of the minimizing solution of Choquard’s nonlinear equation, Stud. Appl. Math. 57, 93 (1977).
  16. I. M. Moroz, R. Penrose, and P. Tod, Spherically-symmetric solutions of the Schrödinger–Newton equations, Classical Quantum Gravity 15, 2733 (1998).
  17. P.-H. Chavanis, Mass-radius relation of Newtonian self-gravitating Bose-Einstein condensates with short-range interactions. I. Analytical results, Phys. Rev. D 84, 043531 (2011).
  18. P.-H. Chavanis and L. Delfini, Mass-radius relation of Newtonian self-gravitating Bose-Einstein condensates with short-range interactions. II. Numerical results, Phys. Rev. D 84, 043532 (2011).
  19. T. D. Lee and Y. Pang, Fermion soliton stars and black holes, Phys. Rev. D 35, 3678 (1987).
  20. M. B. Wise and Y. Zhang, Stable bound states of asymmetric dark matter, Phys. Rev. D 90, 055030 (2014).
  21. L. Del Grosso, G. Franciolini, P. Pani, and A. Urbano, Fermion soliton stars, Phys. Rev. D 108, 044024 (2023).
  22. S. Coleman, Q-balls, Nucl. Phys. B262, 263 (1985).
  23. S. Tulin and H.-B. Yu, Dark matter self-interactions and small scale structure, Phys. Rep. 730, 1 (2018).
  24. D. E. Kaplan, G. Z. Krnjaic, K. R. Rehermann, and C. M. Wells, Atomic dark matter, J. Cosmol. Astropart. Phys. 05 (2010) 021.
  25. W. H. Press and D. N. Spergel, Capture by the Sun of a galactic population of weakly interacting, massive particles, Astrophys. J. 296, 679 (1985).
  26. A. Gould, Weakly interacting massive particle distribution in and evaporation from the sun, Astrophys. J. 321, 560 (1987).
  27. M. T. Frandsen and S. Sarkar, Asymmetric dark matter and the Sun, Phys. Rev. Lett. 105, 011301 (2010).
  28. M. Taoso, F. Iocco, G. Meynet, G. Bertone, and P. Eggenberger, Effect of low mass dark matter particles on the Sun, Phys. Rev. D 82, 083509 (2010).
  29. I. P. Lopes and J. Silk, Solar neutrinos: Probing the quasi-isothermal solar core produced by supersymmetric dark matter particles, Phys. Rev. Lett. 88, 151303 (2002).
  30. I. Lopes and J. Silk, Dark matter burning in nuclear star clusters, Astrophys. J. Lett. 733, L51 (2011).
  31. I. Lopes and J. Silk, Solar constraints on asymmetric dark matter, Astrophys. J. 757, 130 (2012).
  32. I. Lopes and J. Silk, A particle dark matter footprint on the first generation of stars, Astrophys. J. 786, 25 (2014).
  33. I. Lopes, K. Kadota, and J. Silk, Constraint on light dipole dark matter from helioseismology, Astrophys. J. Lett. 780, L15 (2014).
  34. I. Lopes, P. Panci, and J. Silk, Helioseismology with long-range dark matter-baryon interactions, Astrophys. J. 795, 162 (2014).
  35. J. Lopes, I. Lopes, and J. Silk, Asteroseismology of red clump stars as a probe of the dark matter content of the galaxy central region, Astrophys. J. Lett. 880, L25 (2019).
  36. J. Casanellas and I. Lopes, Towards the use of asteroseismology to investigate the nature of dark matter, Mon. Not. R. Astron. Soc. 410, 535 (2011).
  37. J. Casanellas and I. Lopes, First asteroseismic limits on the nature of dark matter, Astrophys. J. Lett. 765, L21 (2013).
  38. J. Rato, J. Lopes, and I. Lopes, On asymmetric dark matter constraints from the asteroseismology of a subgiant star, Mon. Not. R. Astron. Soc. 507, 3434 (2021).
  39. A. de Lavallaz and M. Fairbairn, Neutron stars as dark matter probes, Phys. Rev. D 81, 123521 (2010).
  40. C. Kouvaris and P. Tinyakov, Constraining asymmetric dark matter through observations of compact stars, Phys. Rev. D 83, 083512 (2011).
  41. J. Bramante and N. Raj, Dark matter in compact stars, Phys. Rep. 1052, 1 (2024).
  42. G. Panotopoulos, Á. Rincón, and I. Lopes, Anisotropic dark energy stars within vanishing complexity factor formalism: Hydrostatic equilibrium, radial oscillations, and observational implications, Phys. Lett. B 856, 138901 (2024).
  43. Z. Buras-Stubbs and I. Lopes, Rotational behavior of exotic compact objects, Phys. Rev. D 113, 043049 (2026).
  44. E. Madelung, Quantentheorie in hydrodynamischer form, Z. Phys. 40, 322 (1927).
  45. D. Bohm, A suggested interpretation of the quantum theory in terms of “hidden” variables. I, Phys. Rev. 85, 166 (1952).
  46. C. F. von Weizsäcker, Zur Theorie der Kernmassen, Z. Phys. 96, 431 (1935).
  47. A. Y. Potekhin, A. I. Chugunov, N. N. Shchechilin, and N. Chamel, On variational trial functions in extended Thomas–Fermi method, Phys. Usp. 68, 691 (2025).
  48. G. Manfredi and F. Haas, Self-consistent fluid model for a quantum electron gas, Phys. Rev. B 64, 075316 (2001).
  49. D. Michta, F. Graziani, and M. Bonitz, Quantum hydrodynamics for plasmas: A Thomas–Fermi theory perspective, Contrib. Plasma Phys. 55, 437 (2015).
  50. A. Prsa, P. Harmanec, G. Torres, E. Mamajek, M. Asplund, N. Capitaine, J. Christensen-Dalsgaard, E. Depagne, M. Haberreiter, S. Hekker et al., Nominal values for selected solar and planetary quantities: IAU 2015 resolution B3, Astron. J. 152, 41 (2016).
  51. B. D. Serot and J. D. Walecka, Recent progress in quantum hadrodynamics, Int. J. Mod. Phys. E 6, 515 (1997).
  52. S. Weinberg, Gravitation and Cosmology: Principles and Applications of the General Theory of Relativity (John Wiley & Sons, New York, 1972).
  53. C. M. Will, Theory and Experiment in Gravitational Physics, 2nd ed. (Cambridge University Press, Cambridge, England, 2018), 10.1017/9781316338612.
  54. Z. A. Moldabekov, M. Bonitz, and T. S. Ramazanov, Theoretical foundations of quantum hydrodynamics for plasmas, Phys. Plasmas 25, 031903 (2018).
  55. S. Chandrasekhar, An Introduction to the Study of Stellar Structure (University of Chicago Press, Chicago, 1939).
  56. S. L. Shapiro and S. A. Teukolsky, Black Holes, White Dwarfs, and Neutron Stars: The Physics of Compact Objects (Wiley, New York, 1983), 10.1002/9783527617661.
  57. M. Colpi, S. L. Shapiro, and I. Wasserman, Boson stars: Gravitational equilibria of self-interacting scalar fields, Phys. Rev. Lett. 57, 2485 (1986).
  58. F. S. Guzmán and L. A. Ureña-López, Evolution of the Schrödinger-Newton system for a self-gravitating scalar field, Phys. Rev. D 69, 124033 (2004).
  59. Z. A. Moldabekov, T. Schoof, P. Ludwig, M. Bonitz, and T. S. Ramazanov, Statically screened ion potential and Bohm potential in a quantum plasma, Phys. Plasmas 22, 044501 (2015).
  60. Z. A. Moldabekov, M. Bonitz, and T. S. Ramazanov, Gradient correction and Bohm potential for two- and one-dimensional electron gases at a finite temperature, Contrib. Plasma Phys. 58, 290 (2018).
  61. R. E. Wyatt, Quantum Dynamics with Trajectories. Introduction to Quantum Hydrodynamics (Springer, New York, 2005), 10.1007/0-387-28145-2.
  62. C. L. Gardner and C. Ringhofer, Smooth quantum potential for the hydrodynamic model, Phys. Rev. E 53, 157 (1996).
  63. P.-H. Chavanis, Statistical mechanics of self-gravitating systems in general relativity: I. The quantum Fermi gas, Eur. Phys. J. Plus 135, 290 (2020).
  64. E. Seidel and W.-M. Suen, Oscillating soliton stars, Phys. Rev. Lett. 66, 1659 (1991).
  65. E. Seidel and W.-M. Suen, Formation of solitonic stars through gravitational cooling, Phys. Rev. Lett. 72, 2516 (1994).
  66. M. Maggiore, Gravitational Waves: Volume 1: Theory and Experiments (Oxford University Press, Oxford, 2007).
  67. P. Amaro-Seoane, H. Audley, S. Babak et al., Laser interferometer space antenna, arXiv:1702.00786.
  68. M. Punturo, M. Abernathy, F. Acernese et al., The Einstein telescope: A third-generation gravitational wave observatory, Classical Quantum Gravity 27, 194002 (2010).
  69. D. Reitze, R. X. Adhikari, S. Ballmer et al., Cosmic explorer: The U.S. contribution to gravitational-wave astronomy beyond LIGO, Bull. Am. Astron. Soc. 51, 35 (2019).
  70. S. Kawamura, M. Ando, N. Seto et al., The Japanese space gravitational wave antenna: DECIGO, Classical Quantum Gravity 28, 094011 (2011).
  71. G. M. Harry, P. Fritschel, D. A. Shaddock, W. Folkner, and E. S. Phinney, Laser interferometry for the big bang observer, Classical Quantum Gravity 23, 4887 (2006).
  72. A. Udalski, M. K. Szymański, and G. Szymański, OGLE-IV: Fourth Phase of the optical gravitational lensing experiment, Acta Astron. 65, 1 (2015).
  73. P. Mróz, A. Udalski, J. Skowron, R. Poleski, S. Kozłowski, M. K. Szymański, I. Soszyński, Ł. Wyrzykowski, P. Pietrukowicz, K. Ulaczyk et al., No large population of unbound or wide-orbit Jupiter-mass planets, Nature (London) 548, 183 (2017).
  74. I. A. Bond, F. Abe, R. J. Dodd et al., Real-time difference imaging analysis of MOA Galactic bulge observations during 2000, Mon. Not. R. Astron. Soc. 327, 868 (2001).
  75. C. Alcock, R. A. Allsman, D. R. Alves, T. S. Axelrod, A. C. Becker, D. P. Bennett, K. H. Cook, N. Dalal, A. J. Drake, K. C. Freeman et al., The MACHO project: Microlensing results from 5.7 years of large magellanic cloud observations, Astrophys. J. 542, 281 (2000).
  76. P. Tisserand, L. Le Guillou, C. Afonso, J. N. Albert, J. Andersen, R. Ansari, É. Aubourg, P. Bareyre, J. P. Beaulieu, X. Charlot et al., Limits on the macho content of the galactic halo from the EROS-2 survey of the magellanic clouds, Astron. Astrophys. 469, 387 (2007).
  77. H. Niikura, M. Takada, N. Yasuda, R. H. Lupton, T. Sumi, S. More, T. Kurita, S. Mukae, and M. Oguri, Microlensing constraints on primordial black holes with Subaru/HSC Andromeda observations, Phys. Rev. D 97, 023518 (2018).
  78. C. Y. Lam, J. R. Lu, A. Udalski, I. Bond, D. P. Bennett, J. Skowron, P. Mróz, and R. Poleski, An isolated mass-gap black hole or neutron star detected with astrometric microlensing, Astrophys. J. Lett. 933, L23 (2022).
  79. J. A. Dror, H. Ramani, T. Trickle, and K. M. Zurek, Pulsar timing probes of primordial black holes and subhalos, Phys. Rev. D 100, 023003 (2019).
  80. A. Arvanitaki and S. Dubovsky, Exploring the string axiverse with precision black hole physics, Phys. Rev. D 83, 044026 (2011).
  81. R. Brito, V. Cardoso, and P. Pani, Superradiance: New Frontiers in Black Hole Physics, 2nd ed., Lect. Notes Phys. Vol. 971 (Springer, New York, 2020).
  82. W. G. Unruh, Second quantization in the Kerr metric, Phys. Rev. Lett. 31, 1265 (1973).
  83. D.-C. Dai and D. Stojkovic, Shedding new light on the absence of fermionic superradiance and maximal infalling rate of fermions into a black hole, Phys. Rev. D 108, 084024 (2023).
  84. S. Tremaine and J. E. Gunn, Dynamical role of light neutral leptons in cosmology, Phys. Rev. Lett. 42, 407 (1979).
  85. H. Davoudiasl, P. B. Denton, and D. A. McGady, Ultralight fermionic dark matter, Phys. Rev. D 103, 055014 (2021).
  86. N. Bar, K. Blum, and C. Sun, Galactic rotation curves versus ultralight dark matter: A systematic comparison with SPARC data, Phys. Rev. D 105, 083015 (2022).
  87. C. Di Paolo, F. Nesti, and F. L. Villante, Phase space mass bound for fermionic dark matter from dwarf spheroidal galaxies, Mon. Not. R. Astron. Soc. 475, 5385 (2018).
  88. M. Filzinger, R. Lange, N. Huntemann, C. Sanner, and E. Peik, Improved limits on the coupling of ultralight bosonic dark matter to photons from optical-clock comparisons, Phys. Rev. Lett. 134, 031001 (2025).
  89. E. W. Kolb and I. I. Tkachev, Axion miniclusters and Bose stars, Phys. Rev. Lett. 71, 3051 (1993).
  90. D. G. Levkov, A. G. Panin, and I. I. Tkachev, Gravitational Bose-Einstein condensation in the kinetic regime, Phys. Rev. Lett. 121, 151301 (2018).
  91. B. Eggemeier and J. C. Niemeyer, Formation and mass growth of dark matter halos in fuzzy dark matter simulations, Phys. Rev. D 100, 063528 (2019).

Outline

Information

Sign In to Your Journals Account

Filter

Filter

Article Lookup

Enter a citation